Time of Flight using flight path and radius (Kepler's Equation)

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Discussion Overview

The discussion revolves around calculating the time of flight for a lunar probe given specific parameters such as escape speed, flight path angle, and distances to the moon. The context includes theoretical aspects of orbital mechanics and the application of Kepler's equations.

Discussion Character

  • Homework-related
  • Technical explanation
  • Exploratory

Main Points Raised

  • One participant states the problem involves a lunar probe with escape speed at an altitude of 0.25 DU and a flight path angle of 30°, seeking to determine the time to reach the moon's vicinity (60 DU).
  • Another participant proposes a solution using a Hohmann Transfer approach, calculating the eccentricity based on the apoapsis radius and periapsis radius, leading to a semi-major axis calculation.
  • A third participant notes that since the probe is given escape speed, it will not have a closed orbit, indicating a parabolic trajectory.
  • A later reply suggests that knowing the radial distance, speed, and flight path angle allows for the determination of specific angular momentum and the length of the latus rectum, which can be used to find the time of flight between two true anomaly values.
  • One participant expresses satisfaction after realizing the importance of eccentric anomaly in solving the problem correctly.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between flight path and time of flight, with some proposing specific methods while others challenge or refine those approaches. No consensus is reached on a single method for calculating the time of flight.

Contextual Notes

Participants mention various assumptions, such as the gravitational parameter and the nature of the trajectory (parabolic), which may affect the calculations. There are unresolved elements regarding the application of certain equations and the implications of the flight path angle.

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Homework Statement

A lunar probe is given just escape speed at an altitude of .25 DU and flight path angle 30°. How long will it take the probe to get to the vicinity of the moon (r = 60 DU), disregarding the moon's gravity?

Circular orbit, radius = 1.25 DU
θ = 30°
gravitational parameter = μ = 1 DU^3/TU^2
true anomaly = v
Eccentric Anomaly = E
eccentricity = e
t-to = Time of flight
a = semi-major axis

Homework Equations

Escape velocity = √(2μ/r) = 1.26 DU/TU
tan(θ) = (esin v)/(1 + ecos v)
tan (v/2) = √((1+e)/(1-e))tan(E/2)
t-to = √(a^3/μ)(2k(pi) + (E-esinE) - (Eo - esinEo))
θ(parabolic) = v/2

The Attempt at a Solution


The answer is 223.2TU
I just can't see how flight path relates to time of flight. The second equation in the relevant equations section seems like it would fit for equating flight path and true anomaly but I can't separate the true anomaly variable. I'm not sure if that last equation for a parabolic flight path applies (the orbit is parabolic but I don't know). Any help would be greatly appreciated.
 
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So I'll post a solution I've been working on:

I'm not sure how to think of flight path, but I assumed the transfer maneuver was like a Hohmann Transfer with 60 DU forming the apoapsis radius:
e = (60-1.25)/(60 + 1.25) = .9592

Now I'm trying to find the semi-major axis from the periapsis radius
Rp = a(1-e)
a = Rp/(1-e) = 1.25/(1-.9592) = 30.625 DU

Assuming the probe reaches the Moon's vicinity at apoapsis radius, E = pi and:
t-to = √(30.625^3)(pi - sin pi) = 532 TU
 
If the probe is given escape speed at some point, it will not have a closed orbit; it'll be parabolic.
 
Okay, some hints.

If you know the radial distance, speed, and flight path angle at some instant then you can determine the specific angular momentum h of the probe. That, in turn, gives you the length of the latus rectum p (since you also know the gravitational parameter μ by assumption). The eccentricity is a given since you know that the probe has escape speed. That means you can write the general equation for the conic orbit radius:

## r = \frac{p}{1 + e cos(\nu)}##

and can solve for the two values of ##\nu## involved (at 1.25DU and 60DU). You should be able to work out the time of flight between those two values of true anomaly.

Extra hint: The parabolic eccentric anomaly will be helpful.
 
Awesome, I got the right answer! Thanks so much, I had completely forgot eccentric anomaly was solved differently depending on the orbit/trajectory.
 

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